Let P - given point.
Coordinate x of P = 0.
Coordinate x of m = x.
Then F = − k x F = -kx F = − k x , so
m a = − k x m a + k x = 0 m x ¨ + k x = 0 ma = -kx \\
ma + kx = 0 \\
m\ddot{x} + kx = 0 ma = − k x ma + k x = 0 m x ¨ + k x = 0
We have linear differential equation,
Characteristic equation:
m α 2 + k = 0 α = ± i ⋅ ω , ω = k m m{\alpha}^2 + k = 0 \\
\alpha = \pm i \cdot \omega,
\omega = \sqrt{\frac{k}{m}} m α 2 + k = 0 α = ± i ⋅ ω , ω = m k
So
x = C 1 ⋅ e t α 1 + C 2 ⋅ e t α 2 = C 1 ( e i t ω ) + C 2 ( e − i t ω ) x = C_1 \cdot e^{t\alpha_1} + C_2 \cdot e^{t\alpha_2} = C_1(e^{it\omega})+C_2(e^{-it\omega}) x = C 1 ⋅ e t α 1 + C 2 ⋅ e t α 2 = C 1 ( e i t ω ) + C 2 ( e − i t ω )
with Euler's formula:
x = C 1 ( cos ( ω t ) + i sin ( ω t ) ) + C 2 ( cos ( − ω t ) + i sin ( − ω t ) ) x = C_1(\cos(\omega t) + i\sin(\omega t)) + C_2(\cos(-\omega t) + i\sin(-\omega t)) x = C 1 ( cos ( ω t ) + i sin ( ω t )) + C 2 ( cos ( − ω t ) + i sin ( − ω t ))
x = ( C 1 + C 2 ) c o s ( ω t ) ) + ( i C 1 − i C 2 ) ( s i n ( ω t ) ) x = (C_1 + C_2)cos(\omega t)) + (iC_1 - iC_2)(sin(\omega t)) x = ( C 1 + C 2 ) cos ( ω t )) + ( i C 1 − i C 2 ) ( s in ( ω t ))
Let:
C 1 + C 2 = C 3 i C 1 + i C 2 = C 4 C 3 2 + C 4 2 = A C_1 + C_2 = C_3 \\
iC_1 + iC_2 = C_4 \\
\sqrt{C_3^2+C_4^2} = A \\ C 1 + C 2 = C 3 i C 1 + i C 2 = C 4 C 3 2 + C 4 2 = A
Then:
( C 3 A ) 2 + ( C 4 A ) 2 = 1 C 3 A = sin ϕ C 4 A = cos ϕ (\frac{C_3}{A})^2 + (\frac{C_4}{A})^2 = 1 \\
\frac{C_3}{A} = \sin \phi \\
\frac{C_4}{A} = \cos \phi ( A C 3 ) 2 + ( A C 4 ) 2 = 1 A C 3 = sin ϕ A C 4 = cos ϕ
x = C 3 cos ( ω t ) + C 4 sin ( ω t ) x = C_3\cos(\omega t) + C_4\sin(\omega t) x = C 3 cos ( ω t ) + C 4 sin ( ω t )
x = A ( sin ϕ cos ( ω t ) + cos ϕ sin ( ω t ) ) x = A(\sin \phi \cos(\omega t) + \cos \phi \sin(\omega t)) x = A ( sin ϕ cos ( ω t ) + cos ϕ sin ( ω t ))
x = A sin ( ω t + ϕ ) x = A\sin(\omega t + \phi) x = A sin ( ω t + ϕ ) - harmonic motion equation.
Comments